Physics · lesson 1 of 4
Rotational dynamics and rolling constraints
Angular velocity is the time derivative of angular displacement. For a fixed axis and constant moment of inertia, net torque equals I times angular acceleration.
Learn the ideas
Prerequisites: Newtonian mechanics, derivatives and energy.
Rotation
Angular velocity is the time derivative of angular displacement. For a fixed axis and constant moment of inertia, net torque equals I times angular acceleration.
Energy
Rigid-body rotation about a fixed axis has kinetic energy Iω²/2. A rolling body generally has both translational and rotational kinetic energy.
Constraints
For rolling without slipping, the centre speed equals Rω. That kinematic condition does not imply friction always dissipates energy.
Model limits
The moment of inertia depends on mass distribution and the chosen axis. A point-mass formula cannot replace the inertia of an extended object without justification.
Worked examples
A fixed-axis rotor has I=3 kg m² and net torque 12 N m. Find its angular acceleration.
Use angular acceleration = torque/I = 12/3.
4 rad/s²
A rotor with I=2 kg m² spins at 5 rad/s. Find its rotational kinetic energy.
K=Iω²/2=(2)(25)/2.
25 J
Check your understanding
8 questionsDecimals or fractions are accepted for numeric answers. Proofs and written responses use sample answers and require human marking. This is practice, not a protected examination.
Further reading and review references
These are reference links, not copied exercises, institutional endorsement or proof of independent review.